1. WG6 Activities Conveners : Riccardo Faccini, Antonio Polosa Riccardo Faccini, Antonio Polosa Conveners : Riccardo Faccini, Antonio Polosa Riccardo Faccini, Antonio Polosa SPECTROSCOPY Other physics EXOTICA

2. 2 Valencia SUMMARY M(MeV) J PC (2S+1) L J Open charm thr.  (3770)  (4040)  (4160) (pot. Models) cc ’c’c J/  ’’  c2  c1  c0 hchc X Z X,Y X(3872) the best tetraquark candidate Updated properties  (4415) The 1 -- family: Charmonia, tetraquarks, molecules, hybrids?!? News on the 3940 family + updates on Y(nS)  Y(mS) transitions Yet another particle: X(4160) [  c (3S)?] Z(4430): the first charged state

3. 3 The observation matrix J/     D (*) D (*) J/  J/      (2S)  J/  K,   S  J/  J/  Notes Mass range for B Low stat Only B dec Mass range! No ISR No  0 No Search No B- dec Only B dec Mass windo w X(3872)SeenSeen Not seen No search N/A Not seen Seen Y(3940) No search X(3940) ? Seen No search Not seen No search No Fit No fit Y(4260)Seen No search Not seen No fit N/A Y(4350) Not seen No fit No search Seen No fit N/A Z(4430) No search No fit No search Seen No Fit No searc h Y(4660) Not seen No fit No search Seen No Fit N/A

4. 4 Comments & Perspectives @valencia A branch of physics where there is evidence that something ‘new’ is going onA branch of physics where there is evidence that something ‘new’ is going on Deserves full investigation!Deserves full investigation! Need to observe as many modes as possible in a large range of massesNeed to observe as many modes as possible in a large range of masses Most of the non bserved modes have low  BF. Assuming one wants to reach at least those modes with a BF~0.1 max(BF) and  BF~0.1max(  BF), one needs at least 1000 times more stat.Most of the non bserved modes have low  BF. Assuming one wants to reach at least those modes with a BF~0.1 max(BF) and  BF~0.1max(  BF), one needs at least 1000 times more stat. Could exploit the possibility to scan in energyCould exploit the possibility to scan in energy A long way before the panorama is clarified.A long way before the panorama is clarified. The BF picture still needs to be clarifiedThe BF picture still needs to be clarified SuperB might be needed to say the final wordSuperB might be needed to say the final word Work to be done, starting from this workshopWork to be done, starting from this workshop Systematic definition of theory predictions in the most credited modelsSystematic definition of theory predictions in the most credited models Collection of material on current results in order to sharpen the case for ‘new’ phenomenaCollection of material on current results in order to sharpen the case for ‘new’ phenomena Study of the impact of a SuperBF on this picture, in the context of its competitorsStudy of the impact of a SuperBF on this picture, in the context of its competitors

5. News on spectroscopy Two more charged particles

6. News from spectroscopy Energy scan perfomed by PEP-IIEnergy scan perfomed by PEP-II Test of techniques for eventual SuperB scan in the cc~ area (or above 11.2 GeV?)Test of techniques for eventual SuperB scan in the cc~ area (or above 11.2 GeV?)

7. Overview OF DEVELOPMENTS Three directions 1.Interplay and complementarity with other experiments TODAY: PandaTODAY: Panda 2.Experimental effects  full simulation 3.Other physics TODAY:TODAY: Higgs searchesHiggs searches Decoherence and CPTDecoherence and CPT Talks from D. Bettoni, D. Bugg, and G. Cibinetto Talks from M. A. Sanchis-Lozano and A. Di Domenico

8. Panda at FAIR pp annihilations

9. Panda Plan: Sit at high energy make a survey of states Perform scans in most interesting points

10. Panda vs superb (I) Common coverage of all chamonium states (up to sqrt(s)~5GeV)Common coverage of all chamonium states (up to sqrt(s)~5GeV) Panda very suited for measurement of widths and form factors: eccellent center of mass resolutionPanda very suited for measurement of widths and form factors: eccellent center of mass resolution  c width measurement at E835

11. 11 Panda vs superb (II) (2S+1) L J J PC B-Factories better suited to low L and 1-- pp annihilations better suited to lower states (narrower) Still need to compare yields on same footing!

12. Simulation NEEDS Valentina Santoro has agreed to run some simulationsValentina Santoro has agreed to run some simulations The goal is to have enough statistics to have unmistakable signals (full reco)The goal is to have enough statistics to have unmistakable signals (full reco) Relatively little dependence on detector performancesRelatively little dependence on detector performances We just need to be sure nothing is worsened too much wrt BaBarWe just need to be sure nothing is worsened too much wrt BaBar Critical need: machine backgroundCritical need: machine background Major worries: ISR reconstruction (missing mass) and neutralsMajor worries: ISR reconstruction (missing mass) and neutrals Choise of modes to simulate (~50K each):Choise of modes to simulate (~50K each): e+e-  Y  ISR, Y  D s (*) D s (*) [most interesting final state and testing ISR]e+e-  Y  ISR, Y  D s (*) D s (*) [most interesting final state and testing ISR] B0  X+K-, X+  J/  testing PID and  reco B0  X+K-, X+  J/  testing PID and  reco  Time scale: end of yearTime scale: end of year

13. SuperB Workshop Warwick April 14-17, 2009 Miguel-Angel Sanchis-Lozano IFIC-Valencia 13 Sensitivity to little Higgs Update since Valencia All constraints from B-physics, LEP and g-2 using NMSSMtools All constraints from B-physics, LEP and g-2 using NMSSMtools [hep-ph/0406215], including the recent discovery of the  b (1S) [hep-ph/0406215], including the recent discovery of the  b (1S) state by BaBaR state by BaBaR More complete expressions on branching ratios taking into account More complete expressions on branching ratios taking into account the mixing of pseudoscalar Higgs A 1 with all  b (nS) states the mixing of pseudoscalar Higgs A 1 with all  b (nS) states below open bottom threshold (n=1, 2, 3). below open bottom threshold (n=1, 2, 3). 2-sigma region of discovery in a X d - M A1 plot is shown 2-sigma region of discovery in a X d - M A1 plot is shown We have incorporated in our study (arXiv:0810.4763 [hep-ph]): Method: search for Y(nS)  A  -->  exclusive reco lepton universality in YnS) decays

14. SuperB Workshop Warwick April 14-17, 2009 Miguel-Angel Sanchis-Lozano IFIC-Valencia 14 Conclusions What if... What if... there exists a light CP-odd Higgs of about 10 GeV? there exists a light CP-odd Higgs of about 10 GeV? We have checked that current BLEP bounds can be evaded in the NMSSM We have checked that current BLEP bounds can be evaded in the NMSSM A high luminosity B factory is the ideal place to discover/study such a light Higgs boson using  Υ(nS) ( n=1,2,3) by looking at - decay into τ + τ - (  ): Lepton universality test - decay into τ + τ - (  ): Lepton universality test - direct searches for monochromatic photons (1- or 2-peak scenario) - direct searches for monochromatic photons (1- or 2-peak scenario) - decay into hadrons via the   b0 component of the A 1 - decay into hadrons via the   b0 component of the A 1 Higher states like  Υ(4S) could be considered at a Super B factory Related topics: B s decay, muon g-2 anomaly, light dark matter … Difficult but not impossible discovery scenario for a light A 1 at the LHC Moreover Higgses other than the light pseudoscalar would be at LHC reach! Moreover Higgses other than the light pseudoscalar would be at LHC reach! The seek of the A 1 boson can be seen as complementary/prior to other searches to be performed at the LHC/ILC searches to be performed at the LHC/ILC In progress

15. CPTV and quantum coherence New topic [Not so sure how much it belongs to this WG… ] New topic [Not so sure how much it belongs to this WG… ] Talk from A. Di Domenico (KLOE) on applications to B- Physics of Kaon studiesTalk from A. Di Domenico (KLOE) on applications to B- Physics of Kaon studies Possible CPT Violation:Possible CPT Violation: 1) in eigenstate definition

16. Possible CPTV 2)

17. 3)

19. SuperB sensitivity @B-Factories: time dependence of doubly tagged events

20. PATH TO TDR SPECTROSCOPY Other physics EXOTICA Refine the case adding efficiencies include complementarity with other experiments Are we missing anything? Ideas are welcome! Only one open thread.. Anything more?